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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements TRACE ancillary: a highly-segmented silicon-pad detector for light charged particles emitted in direct nuclear reactions Daniele Mengoni Università e Sezione INFN di Padova ITALIA DREB07, RIKEN, Japan May 30 ÷ June 2, 2007

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  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    TRACE ancillary:a highly-segmented silicon-pad detector

    for light charged particles emitted indirect nuclear reactions

    Daniele MengoniUniversità e Sezione INFN di Padova

    ITALIA

    DREB07, RIKEN, JapanMay 30 ÷ June 2, 2007

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Outline

    1 Introduction

    2 TRACE simulation and designEstimations, simulation and performances evaluationSignals induced in silicon

    3 Experimental testsIn beam test: silicon ancillary coupled to the AGATA clusterDetector & electronics (NIM, ASIC) tests

    4 Conclusion

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Introduction

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    IntroductionInstrumentation: γ-spectrometers

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    IntroductionInstrumentation: ancillaries used in conjunction with γ-spectrometers

    Selectivity improvement and background reduction

    PRISMA

    DANTE

    MICROBALL

    TIARAMUST2

    EUCLIDES

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    IntroductionSuitable reactions

    Direct nuclear reactionsin inverse kinematics to measure the angle of the recoiling lightparticle.

    ... Fusion-evaporation reactionsto measure energy and angle of the recoiling light particle withancillary detectors coupled with gamma arrays.

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    IntroductionSuitable reactions

    Direct nuclear reactionsin inverse kinematics to measure the angle of the recoiling lightparticle.

    ... Fusion-evaporation reactionsto measure energy and angle of the recoiling light particle withancillary detectors coupled with gamma arrays.

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Design criteria

    Guidelines

    Material Transparency, energy resolution,properties, costs

    Particle discriminationtechnique

    Segmentation

    Efficiency

    Pad (or strips)

    4π detector

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Design criteria

    Guidelines

    MaterialParticle discriminationtechnique E-∆E, thickness

    Segmentation

    Efficiency

    Pad (or strips)

    4π detector

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Design criteria

    Guidelines

    Material

    Particle discriminationtechniqueSegmentation Angular resolution

    Efficiency

    Pad (or strips)

    4π detector

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Design criteria

    Guidelines

    Material

    Particle discriminationtechnique

    SegmentationEfficiency Solid angle coverage, lowenergy threshold

    Pad (or strips)

    4π detector

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Design criteria

    Guidelines

    Material

    Particle discriminationtechnique

    Segmentation

    EfficiencyPad (or strips) Sizable number, heatdissipation, energy resolution

    4π detector

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Design criteria

    Guidelines

    Material

    Particle discriminationtechnique

    Segmentation

    Efficiency

    Pad (or strips)4π detector Reaction kinematics

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Simulation: frameworkEvent generator, radiation interaction, filter (PSA, tracking), data collection (matricesand spectra)

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Simulation: frameworkEvent generator, radiation interaction, filter (PSA, tracking), data collection (matricesand spectra)

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Simulation: frameworkEvent generator, radiation interaction, filter (PSA, tracking), data collection (matricesand spectra)

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Simulation: frameworkEvent generator, radiation interaction, filter (PSA, tracking), data collection (matricesand spectra)

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Simulation: frameworkEvent generator, radiation interaction, filter (PSA, tracking), data collection (matricesand spectra)

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Simulation: frameworkEvent generator, radiation interaction, filter (PSA, tracking), data collection (matricesand spectra)

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Simulation: TRACETRacking Array for light Charged particle Ejectiles

    Starting point: improvement of the EUCLIDES Si ball;

    Next steps: increase segmentation and solid anglecoverage without losing in simplicity (barrel, end-caps).

    Hodoscope Euclides-like TRACE4,6,8module

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Transparency

    Full-energy eff.:probability to detect the total energy of any emittedphoton individually

    Peak-to-total ratio: the ratio of full energy efficiency to the totalinteraction efficiency.

    Absolute photopeak eff. (%)

    15

    20

    25

    30

    35

    40

    45

    50

    0 500 1000 1500 2000 2500 3000

    Absolute photopeak eff. (%)

    Energy (keV)

    A180A180+Al chamber+EUCLIDESA180+Al chamber+TRACE4A180+Al chamber+TRACE6A180+Al chamber+TRACE8

    Peak-to-total ratio (%)

    0

    20

    40

    60

    80

    100

    0 500 1000 1500 2000 2500 3000

    Peak-to-total ratio (%)

    Energy (keV)

    A180A180+Al chamber+EUCLIDES

    A180+Al chamber+TRACE4+ASICsA180+Al chamber+TRACE6A180+Al chamber+TRACE8

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Doppler correctionTRACE8

    Doppler broadening

    uncertainty in the photon emission angle

    uncertainty in the recoil energy

    intrinsic detector resolution

    2

    2.5

    3

    3.5

    4

    4.5

    5

    5.5

    6

    6.5

    0 1 2 3 4 5 6 7 8

    FWHM (keV)

    Segmentation (mm2)

    transfer v/c=6.4%transfer v/c=7.8%

    0

    0.2

    0.4

    0.6

    0.8

    1

    1.2

    0 20 40 60 80 100 120 140 160 180

    ∆Eγ/E

    γ (%)

    Angle (deg)

    ∆θ = 0.5°∆β = 1%

    v/c=15%v/c=10%v/c= 5%

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Collecting electrodesRear side current signals as a function of the injected particles.The particles are injected in the middle of the central pad.

    α family3_MeV 5_MeV 10_MeV 30_MeV

    Time (s)

    1e−10 1e−09 1e−08 1e−07 1e−06 1e−05

    Cu

    rre

    nt

    (A)

    2e−05

    4e−05

    6e−05

    8e−05

    1e−04

    proton family3_MeV 5_MeV 10_MeV 30_MeV

    Time (s)

    1e−10 1e−09 1e−08 1e−07 1e−06 1e−05

    Cu

    rre

    nt

    (A)

    1e−04

    2e−04

    3e−04

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Neighbour electrodesRear side, bipolar transient signals as a function of the injected particles.The particles are injected in the middle of the central pad.

    α family3_MeV 5_MeV 10_MeV 30_MeV

    Time (s)

    1E−10 1E−9 1E−8 1E−7 1E−6 1E−5

    Cu

    rre

    nt

    (A)

    −3e−06

    −2e−06

    −1e−06

    0

    proton family30_MeV 10_MeV 5_MeV 3_MeV

    Time (s)

    1E−10 1E−9 1E−8 1E−7 1E−6 1E−5

    Cu

    rre

    nt

    (A)

    −2e−06

    0

    2e−06

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Ancillary impactSingle hit on Si, Ge cluster

    Silicon center, PSA on Ge detector

    Full information on the DSSSD, PSA on Ge detector

    AGATA cluster + ancillary 49Ti Energy resolution

    1365 1370 1375 1380 1385 1390 1395

    1000

    2000

    3000

    4000

    5000

    6000

    E_titleCLUSTCORRCAL_pSIpGE

    6.1 keV7.7 keV

    Cou

    nts

    keV

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Preliminary tests: ITC-IRST detectors300 µm,1 mm, 1.5 mm thickness, 1x1, 2x2, 4x4 mm2, low resistivity, AC coupling.

    Junction side: DC, AC pad; biasand reference voltage; guardrings; “punch-through” resistance.

    pad layout zoom

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Preliminary tests: ITC-IRST detectorsEnergy resolution with modular NIM and ASIC electronics

    0

    50

    100

    150

    200

    250

    300

    350

    400

    450

    4800 5000 5200 5400 5600 5800 6000 6200

    Counts

    Energy (keV)

    50 keV

    0

    2000

    4000

    6000

    8000

    10000

    12000

    4800 5000 5200 5400 5600 5800 6000 6200

    Counts

    Energy (keV)

    60 keV

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    ConclusionTelescope Prototype

    ASIC: quasi-parallel energy-time cycle;

    Telescope prototype closely resembles the traditional Sitelescope;

    TRACE prototype key features: Si-pad technology,integrated electronics, high segmentation, PSA ...

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Summary

    Simple estimations

    Geometry simulation

    PSA simulation

    Ancillary impact

    Si and electronics test

    =⇒ telescope specifications and possible prototype.

    Future perspectives:PSA testIn beam test

  • Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements

    Acknowledgements

    INFN (Italy)

    LNL: A. Gadea, G. Prete, G. de Angelis, J.J. Valiente-Dobon,R. Orlandi, F. della Vedova, E. Sahin, R.P. Singh, R. Ponchia,P. Cocconi, D. Rosso.

    Sezione di Padova: F. Recchia, E. Farnea, D.Bazzacco,S.Lunardi, C. Ur, R. Isocrate.

    Sezione di Perugia: E. Fiandrini, G. Ambrosi, M. Ionica,G. Alberti.

    IN2P3 (F)

    C.M. Petrache, P. Edelbruck, L. Lavergne, L. Leterrier, and theMUST2 team.

    Surrey University (UK)

    P.H. Regan and the TIARA team.